LMH7322
LMH7322 Dual 700 ps High Speed Comparator with RSPECL Outputs
Literature Number: SNOSAU8H
LMH7322
May 11, 2011
Dual 700 ps High Speed Comparator with RSPECL Outputs
General Description
The LMH7322 is a dual comparator with 700 ps propagation
delay, low dispersion of 75 ps and an input voltage range that
extends from VCC-1.5V to VEE. The devices can be operated
from a wide supply voltage range of 2.7V to 12V. The ad-
justable hysteresis adds flexibility and prevents oscillations.
Both the outputs and latch inputs of the LMH7322 are
RSPECL compatible. When used in combination with a
VCCO supply voltage of 2.5V the outputs have LVDS compat-
ible levels.
The LMH7322 is available in a 24-pin LLP package.
Features
(VCCI = +5V, VCCO = +5V)
Propagation delay 700 ps
Overdrive dispersion 20 mV-1V 75 ps
Fast rise and fall times 160 ps
Wide supply range 2.7V to 12V
Input common mode range extends 200 mV below
negative rail
Adjustable hysteresis
(RS)PECL outputs (see application note)
(RS)PECL latch inputs (see application note)
Applications
Digital receivers
High-speed signal restoration
Zero-crossing detectors
High-speed sampling
Window comparators
High-speed signal triggering
Typical Application
(RS)ECL to RSPECL Converter
20183205
© 2011 National Semiconductor Corporation 201832 www.national.com
LMH7322 Dual 700 ps High Speed Comparator with RSPECL Outputs
Absolute Maximum Ratings (Note 1)
If Military/Aerospace specified devices are required,
please contact the National Semiconductor Sales Office/
Distributors for availability and specifications.
ESD Tolerance (Note 2)
Human Body Model 2.5 kV
Machine Model 250V
Output Short Circuit Duration (Note 3, Note 4)
Supply Voltages (VCCx–VEE)13.2V
Differential Voltage at Input Pins ±13V
Voltage at Input Pins VEE-0.2V to VCCI + 0.2V
Voltage at LE Pins VEE-0.2V to VCCO+0.2V
Current at Output Pins 25mA
Soldering Information:
See Product Folder at www.national.com and http://
www.national.com/ms/MS/MS-SOLDERING.pdf
Storage Temperature Range −65°C to +150°C
Junction Temperature (Note 7) +150°C
Operating Conditions (Note 1)
Supply Voltage (VCCx–VEE) 2.7V to 12V
Operating Temperature Range
(Note 5, Note 6) −40°C to +125°C
Package Thermal Resistance
(Note 5, Note 6)
24-Pin LLP 38°C/W
12V DC Electrical Characteristics Unless otherwise specified, all limits are guaranteed for TJ = 25°C,
VCCI = VCCO = 12V, VEE = 0V, RL = 50Ω to VCCO-2V, VCM = 300 mV, RHYS = 1 kΩ. Boldface limits apply at temperature extremes.
Symbol Parameter Conditions Min
(Note 8)
Typ
(Note 7)
Max
(Note 8)Units
INPUT CHARACTERISTICS
IBInput Bias Current VIN Differential = 0V; RHYS = 8 k Biased
at VCM
−5 −2.9 µA
IOS Input Offset Current VIN Differential = 0V −250 40 +250 nA
TC IOS Input Offset Current TC VIN Differential = 0V 0.2 nA/°C
VOS Input Offset Voltage −8 −2 +8 mV
TC VOS Input Offset Voltage TC 12 µV/°C
VRI Input Voltage Range for CMRR 50 dB VEE−0.2 VCCI−1.5 V
VRID Input Differential Voltage Range −1 +1 V
CMRR Common Mode Rejection Ratio 0V VCM VCC1−0.2 80 dB
PSRR Power Supply Rejection Ratio 80 dB
AVActive Gain 53 dB
Hyst Hysteresis VHYS = V(HYS+) -V(HYS-) , RHYS = 0Ω 25 50 75 mV
LATCH ENABLE CHARACTERISTICS
IB-LE Latch Enable Bias Current Biased at RSPECL Level 3 10 µA
VOS-LE Latch Enable Offset Voltage Biased at RSPECL Level −5 mV
VRI-LE Latch Enable Voltage Range for CMRR 50 dB VEE+1.4 VCCO-0.8 V
VRID-LE Latch Enable Differential Voltage
Range
±0.4 V
OUTPUT CHARACTERISTICS
VOH Output Voltage High VIN Differential = 50 mV VCCO−1.1V mV
VOL Output Voltage Low VIN Differential = 50 mV VCCO−1.5V mV
VOD Output Voltage Differential VIN Differential = 50 mV 360 mV
POWER SUPPLIES
IVCCI VCCI Supply Current/ Channel 6.5 10
12 mA
IVCCO VCCO Supply Current/ Channel Load Current Excluded 16.3 20
25
mA
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LMH7322
12 AC Electrical Characteristics Unless otherwise specified, all limits are guaranteed for TJ = 25°C,
VCCI = VCCO = 12V, VEE = 0V, RL = 50Ω to VCCO-2V, VCM = 300 mV, RHYS = none.Boldface limits apply at temperature extremes.
Symbol Parameter Conditions Min
(Note 8)
Typ
(Note 7)
Max
(Note 8)Units
TR Maximum Toggle Rate Overdrive = ±50 mV; CL = 2 pF
@ 50% of Output Swing
4 Gb/s
Minimum Pulse Width Overdrive = ±50 mV; CL = 2 pF
@ 50% of Output Swing
255 ps
tjitter-RMS RMS Random Jitter Overdrive = ±100 mV; CL = 2 pF
Center Frequency = 140 MHz
Bandwidth = 10 Hz–20 MHz
702 fs
tPDH Propagation Delay.
(see Figure 3 application note)
Overdrive 20 mV 818 ps
Overdrive 50 mV 723
Input SR = Constant
VIN Startvalue = VREF −100 mV
Overdrive 100 mV 708 ps
Overdrive 1V 703
tOD-disp Input Overdrive Dispersion tPDH @ Overdrive 20 mV 100 mV 110
ps
tPDH @ Overdrive 100 mV 1V 5
tSR-disp Input Slew Rate Dispersion 0.1 V/ns to 1 V/ns; Overdrive = 100 mV 48 ps
tCM-disp Input Common Mode Dispersion SR = 1 V/ns; Overdrive = 100 mV;
0V VCM VCCI- 1.5V
43 ps
ΔtPDLH Q to Q Time Skew |tPDH – tPDL| Overdrive = 100 mV; CL = 2 pF 24 ps
ΔtPDHL Q to Q Time Skew |tPDL – tPDH| Overdrive = 100 mV; CL = 2 pF 45 ps
trOutput Rise Time (20%–80%) Overdrive = 100 mV; CL = 2 pF 155 ps
tfOutput Fall Time (20%–80%) Overdrive = 100 mV; CL = 2 pF 155 ps
tsLE Latch Setup Time 77 ps
thLE Latch Hold Time 33 ps
tPD_LE Latch to Output Delay Time 944 ps
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LMH7322
5V DC Electrical Characteristics Unless otherwise specified, all limits are guaranteed for TJ = 25°C,
VCCI = VCCO = 5V, VEE = 0V, RL = 50Ω to VCCO-2V, VCM = 300 mV, RHYS = 1 kΩ.Boldface limits apply at temperature extremes.
Symbol Parameter Conditions Min
(Note 8)
Typ
(Note 7)
Max
(Note 8)Units
INPUT CHARACTERISTICS
IBInput Bias Current VIN Differential = 0V; RHYS = 8 k
Biased at VCM
−5 −2.6 µA
IOS Input Offset Current VIN Differential = 0V −250 40 +250 nA
TC IOS Input Offset Current TC VIN Differential = 0V 0.3 nA/°C
VOS Input Offset Voltage −8 −2 +8 mV
TC VOS Input Offset Voltage TC 12 µV/°C
VRI Input Voltage Range for CMRR 50 dB VEE−0.2 VCCI−1.5 V
VRID Input Differential Voltage
Range
−1 +1 V
CMRR Common Mode Rejection Ratio 0V VCM VCC1−0.2 80 dB
PSRR Power Supply Rejection Ratio 80 dB
AVActive Gain 53 dB
Hyst Hysteresis VHYS = V(HYS+) -V(HYS-) , RHYS = 0Ω 25 50 75 mV
LATCH ENABLE CHARACTERISTICS
IB-LE Latch Enable Bias Current Biased at RSPECL Level 3 10 µA
VOS-LE Latch Enable Offset Voltage Biased at RSPECL Level +5 mV
VRI-LE Latch Enable Voltage Range for CMRR 50 dB VEE+1.4 VCCO-0.8 V
VRID-LE Latch Enable Differential
Voltage Range
±0.4 V
OUTPUT CHARACTERISTICS
VOH Output Voltage High VCCO−1.1V mV
VOL Output Voltage Low VCCO−1.5V mV
VOD Output Voltage Differential 355 mV
POWER SUPPLIES
IVCCI VCCI Supply Current/ Channel 6.3 10
12
mA
IVCCO VCCO Supply Current/ Channel Load Current Excluded 15.8 20
25
mA
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LMH7322
5V AC Electrical Characteristics Unless otherwise specified, all limits are guaranteed for TJ = 25°C,
VCCI = VCCO = 5V, VEE = 0V, RL = 50Ω to VCCO-2V, VCM = 300 mV, RHYS = none. Boldface limits apply at temperature extremes.
Symbol Parameter Conditions Min
(Note 8)
Typ
(Note 7)
Max
(Note 8)Units
TR Maximum Toggle Rate Overdrive = ±50 mV; CL = 2 pF
@ 50% of Output Swing
3.9 Gb/s
Minimum Pulse Width Overdrive = ±50 mV; CL = 2 pF
@ 50% of Output Swing
260 ps
tjitter_RMS RMS Random Jitter Overdrive = ±100 mV; CL = 2 pF
Center Frequency = 140 MHz
Bandwidth = 10 Hz–20 MHz
572 fs
tPDLH Propagation Delay.
(see Figure 3 application note)
Overdrive 20 mV 783 ps
Overdrive 50 mV 718
Input SR = Constant
VIN startvalue = VREF – 100 mV
Overdrive 100 mV 708 ps
Overdrive 1V 708
tOD-disp Input Overdrive Dispersion tPDH @ Overdrive 20 mV 100 mV 75
ps
tPDH @ Overdrive 100 mV 1V 5
tSR-disp Input Slew Rate Dispersion 0.1 V/ns to 1 V/ns; Overdrive = 100 mV 50 ps
tCM-disp Input Common Mode Dispersion SR = 1 V/ns; Overdrive = 100 mV;
0V VCM VCCI- 1.5V
24 ps
ΔtPDLH Q to Q Time Skew |tPDH – tPDL| Overdrive = 100 mV; CL = 2 pF 29 ps
ΔtPDHL Q to Q Time Skew |tPDL – tPDH| Overdrive = 100 mV; CL = 2 pF 47 ps
trOutput Rise Time (20%–80%) Overdrive = 100 mV; CL = 2 pF 160 ps
tfOutput Fall Time (20%–80%) Overdrive = 100 mV; CL = 2 pF 160 ps
tsLE Latch Setup Time 95 ps
thLE Latch Hold Time 29 ps
tPD_LE Latch to Output Delay Time 893 ps
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LMH7322
2.7V DC Electrical Characteristics Unless otherwise specified, all limits are guaranteed for TJ = 25°C,
VCCI = VCCO = 2.7V, VEE = 0V, RL = 50Ω to VCCO-2V, VCM = 300 mV, RHYS = 1 kΩ. Boldface limits apply at temperature extremes.
Symbol Parameter Conditions Min
(Note 8)
Typ
(Note 7)
Max
(Note 8)Units
INPUT CHARACTERISTICS
IBInput Bias Current VIN Differential = 0V; RHYS = 8 k
Biased at VCM
−5 −2.5 µA
IOS Input Offset Current VIN Differential = 0V −250 40 +250 nA
TC IOS Input Offset Current TC VIN Differential = 0V 0.2 nA/°C
VOS Input Offset Voltage −8 −2 +8 mV
TC VOS Input Offset Voltage TC 12 µV/°C
VRI Input Voltage Range for CMRR 50 dB VEE−0.2 VCCI−1.5 V
VRID Input Differential Voltage
Range
−1 +1 V
CMRR Common Mode Rejection
Ratio
0V VCM VCC1−2 80 dB
PSRR Power Supply Rejection Ratio 80 dB
AVActive Gain 53 dB
Hyst Hysteresis VHYS = V(HYS+) -V(HYS-) , RHYS = 0Ω 25 50 75 mV
LATCH ENABLE CHARACTERISTICS
IB-LE Latch Enable Bias Current Biased at RSPECL Level 3 10 µA
VOS-LE Latch Enable Offset Voltage Biased at RSPECL Level −5 mV
VRI-LE Latch Enable Voltage Range for CMRR 50 dB VEE+1.4 VCCO-0.8 V
VRID-LE Latch Enable Differential
Voltage Range
±0.4 V
OUTPUT CHARACTERISTICS
VOH Output Voltage High VCCO−1.1V mV
VOL Output Voltage Low VCCO−1.5V mV
VOD Output Voltage Differential 350 mV
POWER SUPPLIES
IVCCI VCCI Supply Current/ Channel 6.2 10
12
mA
IVCCO VCCO Supply Current/ Channel Load Current Excluded 15.5 20
25
mA
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LMH7322
2.7V AC Electrical Characteristics Unless otherwise specified, all limits are guaranteed for TJ = 25°C,
VCCI = VCCO = 2.7V, VEE = 0V, RL = 50Ω to VCCO-2V, VCM = 300 mV, RHYS = none. Boldface limits apply at temperature extremes.
Symbol Parameter Conditions Min
(Note 8)
Typ
(Note 7)
Max
(Note 8)Units
TR Maximum Toggle Rate Overdrive = ±50 mV; CL = 2 pF
@ 50% of Output Swing
3.8 Gb/s
Minimum Pulse Width Overdrive = ±50 mV; CL = 2 pF
@ 50% of Output Swing
265 ps
tjitter_RMS RMS Random Jitter Overdrive = ±50 mV; CL = 2 pF
Center Frequency = 140 MHz
Bandwidth = 10 Hz–20 MHz
551 fs
tPDH Propagation Delay.
(see Figure 3 application note)
Overdrive 20 mV 783 ps
Overdrive 50 mV 728
Input SR = Constant
VIN startvalue = VREF – 100 mV
Overdrive 100 mV 713 ps
Overdrive 1V 718
tOD-disp Input Overdrive Dispersion tPDH @ Overdrive 20 mV 100 mV 70
ps
tPDH @ Overdrive 100 mV 1V 5
tSR-disp Input Slew Rate Dispersion 0.1 V/ns to 1 V/ns; Overdrive = 100 mV 54 ps
tCM-disp Input Common Mode
Dispersion
SR = 1 V/ns; Overdrive = 100 mV;
0V VCM VCCI- 1.5V
12 ps
ΔtPDLH Q to Q Time Skew |tPDH – tPDL| Overdrive = 100 mV; CL = 2 pF 35 ps
ΔtPDHL Q to Q Time Skew |tPDL – tPDH| Overdrive = 100 mV; CL = 2 pF 53 ps
trOutput Rise Time (20%–80%) Overdrive = 100 mV; CL = 2 pF 165 ps
tfOutput Fall Time (20%–80%) Overdrive = 100 mV; CL = 2 pF 165 ps
tsLE Latch Setup Time 102 ps
thLE Latch Hold Time 37 ps
tPD_LE Latch to Output Delay Time 906 ps
Note 1: Absolute Maximum Ratings indicate limits beyond which damage to the device may occur. Operating Ratings indicate conditions for which the device is
intended to be functional, but specific performance is not guaranteed. For guaranteed specifications and the test conditions, see the Electrical Characteristics.
Note 2: Human Body Model, applicable std. MIL-STD-883, Method 3015.7. Machine Model, applicable std. JESD22-A115-A (ESD MM std. of JEDEC)
Field-Induced Charge-Device Model, applicable std. JESD22-C101-C (ESD FICDM std. of JEDEC).
Note 3: Applies to both single-supply and split-supply operation. Continuous short circuit operation at elevated ambient temperature can result in exceeding the
maximum allowed junction temperature of 150°C.
Note 4: Short circuit test is a momentary test. See next note.
Note 5: The maximum power dissipation is a function of TJ(MAX), θJA. The maximum allowable power dissipation at any ambient temperature is
PD = (TJ(MAX) – TA)/ θJA. All numbers apply for packages soldered directly onto a PC Board.
Note 6: Electrical Table values apply only for factory testing conditions at the temperature indicated. Factory testing conditions result in very limited self-heating
of the device such that TJ = TA. No guarantee of parametric performance is indicated in the electrical tables under conditions of internal self-heating where TJ >
TA. See Applications section for information on temperature de-rating of this device.
Note 7: Typical values represent the most likely parametric norm as determined at the time of characterization. Actual typical values may vary over time and will
also depend on the application and configuration. The typical values are not tested and are not guaranteed on shipped production material.
Note 8: All limits are guaranteed by testing or statistical analysis.
Note 9: Positive current corresponds to current flowing into the device.
Note 10: Slew rate is the average of the positive and negative slew rate.
Note 11: Average Temperature Coefficient is determined by dividing the change in a parameter at temperature extremes by the total temperature change.
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LMH7322
Connection Diagrams
Schematic
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Footprint
20183201
Ordering Information
Package Part Number Package Marking Transport Media NSC Drawing
24-Pin LLP
NOPB
LMH7322SQ
L7322SQ
1k Units Tape and Reel
SQA24ALMH7322SQE 250 Units Tape and Reel
LMH7322SQX 4.5 Units Tape and Reel
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LMH7322
Typical Performance Characteristics At TJ = 25°C; VCCI = +5V; VCCO = +3.3V; VEE = −5V; unless
otherwise specified.
Propagation Delay vs. Supply Voltage
20183226
Propagation Delay vs. Temperature
20183227
Propagation Delay vs. Supply Voltage
20183228
Propagation Delay vs. Overdrive Voltage
20183229
Propagation Delay vs. Common Mode Voltage
20183230
Propagation Delay vs. Slew Rate
20183231
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LMH7322
TPD Dispersion vs. Supply Voltage
20183232
Slew Rate Dispersion vs. Voltage Supply
20183233
Common Mode Dispersion vs. Supply Voltage
20183234
Bias Current vs. Temperature
20183235
Input Current vs. Differential Input Voltage
20183236
Maximum Toggle Rate
20183237
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LMH7322
Output Voltage vs. Input Voltage
20183238
Hysteresis Voltage vs. Hysteresis Resistor
20183239
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LMH7322
Application Information
INTRODUCTION
The LMH7322 is a high speed comparator with RS(P)ECL
(Reduced Swing Positive Emitter Coupled Logic) outputs,
and is compatible with LVDS (Low Voltage Differential Sig-
naling) if VCCO is set to 2.5V. The use of complementary
outputs gives a high level of suppression for common mode
noise. The very fast rise and fall times of the LMH7322 enable
data transmission rates up to several Gigabits per second
(Gbps). The LMH7322 inputs have a common mode voltage
range that extends 200 mV below the negative supply voltage
thus allowing ground sensing in case of single supply. The
rise and fall times of the LMH7322 are about 160 ps, while the
propagation delay time is about 700 ps. The LMH7322 can
operate over the full supply voltage range of 2.7V to 12V,
while using single or dual supply voltages. This is a very useful
feature because it provides a flexible way to interface be-
tween several high speed logic families. Several setups are
shown in the application information section “INTERFACE
BETWEEN LOGIC FAMILIES”. The outputs are referenced
to the positive VCCO supply rail. The supply current is 23 mA
at 5V (per comparator, load current excluded.) The LMH7322
is available in a 24-Pin LLP package.
The following topics will be discussed in this application sec-
tion.
Input and output topology
Specification definitions
Propagation delay and dispersion
Hysteresis and oscillations
Output
Applying transmission lines
PCB layout
INPUT & OUTPUT TOPOLOGY
All input and output pins are protected against excessive volt-
ages by ESD diodes. These diodes are conducting from the
negative supply to the positive supply. As can be seen in
Figure 1, both inputs are connected to these diodes. Further
protection of the inputs is provided by the two resistors of
250, in conjunction with the string of anti-parallel diodes
connected between both bases of the input stage. This com-
bination of resistors and diodes reduces excessive input volt-
ages over the input stage, but is low enough to maintain
switching speed to the output signal.
Protection against excessive supply voltages is provided by
a power clamp between VCC and GND.
When using this part be aware of situations in which the dif-
ferential input voltage level is such that these diodes are
conducting. In this case the input current is raised far above
the normal value stated in the datasheet tables because input
current is flowing through the bypass diode string between
both inputs.
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FIGURE 1. Equivalent Input Circuitry
The output stage of the LMH7322 is built using two emitter
followers, which are referenced to the VCCO (see Figure 2.)
Each of the output transistors is active when a current is flow-
ing through any external output resistor connected to a lower
supply rail. The output structure is actually the same as for all
other ECL devices. Activating the outputs is done by con-
necting the emitters to a termination voltage which lies 2V
below the VCCO. In this case a termination resistor of 50 can
be used and a transmission line of 50 can be driven. Another
method is to connect the emitters through a resistor to the
most negative supply by calculating the right value for the
emitter current in accordance with the datasheet tables. Both
methods are useful, and it is up to the customer which method
is used. Using 50 to the termination voltage means the in-
troduction of an extra supply in the system, while using resis-
tors to a negative supply means the use of resistors that are
much larger than 50 and a more constant output current per
stage. The following calculation will show the difference. In
this example a VCCO of 2.5V is used and a VT of VCCO-2V and
a negative supply of −5V. When connecting the outputs
through a 50 resistor to the VT, the output currents for the
high and the low state are respectively 18 mA and 10 mA.
Connecting the outputs through a 400 resistor to the −5V
supply the output currents for the high and the low state are
respectively 16 mA and 15 mA. Higher resistor values to the
VEE will further reduce power consumption but will cause a
slower transition of the output stage. In the case that this will
not harm your application it is a useful method to reduce pow-
er consumption.
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LMH7322
20183210
FIGURE 2. Equivalent Output Circuitry
The output voltages for ‘1’ and ‘0’ have a difference of ap-
proximately 400 mV and are respectively 1.1V (for the ‘1’) and
1.5V (for the ‘0’) below the VCCO. This swing of 400 mV is
enough to drive any LVDS input but can also be used to drive
any ECL or PECL input, when the right supply voltage is cho-
sen, especially the right level for the VCCO.
Definitions
Symbol Text Description
IBInput Bias Current Current flowing in or out of the input pins, when both are biased at the VCM
voltage as specified in the tables.
IOS Input Offset Current Difference between the input bias current of the inverting and non-inverting
inputs.
TC IOS Average Input Offset Current Drift Temperature coefficient of IOS.
VOS Input Offset Voltage Voltage difference needed between IN+ and IN- to make the outputs change
state, averaged for H to L and L to H transitions.
TC VOS Average Input Offset Voltage Drift Temperature coefficient of VOS .
VRI Input Voltage Range Voltage which can be applied to the input pin maintaining normal operation.
VRID Input Differential Voltage Range Differential voltage between positive and negative input at which the input
clamp is not working. The difference can be as high as the supply voltage but
excessive input currents are flowing through the clamp diodes and protection
resistors.
CMRR Common Mode Rejection Ratio Ratio of input offset voltage change and input common mode voltage change.
PSRR Power Supply Rejection Ratio Ratio of input offset voltage change and supply voltage change from VS-MIN
to VS-MAX.
AVActive Gain Overall gain of the circuit.
Hyst Hysteresis Difference between the switching point ‘0’ to ‘1’ and vice versa.
IB-LE Latch Enable Bias Current Current flowing in or out of the input pins, when both are biased at normal
PECL levels.
IOS-LE Latch Enable Offset Current Difference between the input bias current of the LE and LE pin.
TC IOS-LE Temp Coefficient Latch Enable Offset
Current
Temperature coefficient of IOS-LE.
VOS-LE Latch Enable Offset Voltage Voltage difference needed between LE and LE to place the part in the latched
or the transparent state.
TC VOS-LE Temp Coefficient Latch Enable Offset
Voltage
Temperature coefficient of VOS-LE.
VRI-LE Latch Enable Voltage Range Voltage which can be applied to the LE input pins without damaging the
device.
VRID-LE Latch Enable Differential Voltage
Range
Differential Voltage between LE and LE at which the clamp isn’t working. The
difference can be as high as the supply voltage but excessive input currents
are flowing through the clamp diodes and protection resistors.
VOH Output Voltage High High state single ended output voltage (Q or Q) (see Figure 18).
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LMH7322
Symbol Text Description
VOL Output Voltage Low Low state single ended output voltage (Q or Q) (see Figure 18).
VOD average of VODH and VODL (VODH + VODL)/2.
IVCCI Supply Current Input Stage Supply current into the input stage.
IVCCO Supply Current Output Stage Supply current into the output stage while current through the load resistors
is excluded.
IVEE Supply Current VEE pin Current flowing to the negative supply pin.
TR Maximum Toggle Rate Maximum frequency at which the outputs can toggle between the nominal
VOH and VOL.
PW Pulse Width Time from 50% of the rising edge of a signal to 50% of the falling edge.
tPDH resp
tPDL
Propagation Delay Delay time between the moment the input signal crosses the switching level
L to H and the moment the output signal crosses 50% of the rising edge of Q
output (tPDH), or delay time between the moment the input signal crosses the
switching level H to L and the moment the output signal crosses 50% of the
falling edge of Q output (tPDL).
tPDL resp
tPDH
Delay time between the moment the input signal crosses the switching level
L to H and the moment the output signal crosses 50% of the falling edge of
Q output (tPDL), or delay time between the moment the input signal crosses
the switching level H to L and the moment the output signal crosses 50% of
the rising edge of Q output (tPDH).
tPDLH Average of tPDH and tPDL .
tPDHL Average of tPDL and tPDH.
tPD Average of tPDLH and tPDHL.
tPDHd resp
tPDLd
Delay time between the moment the input signal crosses the switching level
L to H and the zero crossing of the rising edge of the differential output signal
(tPDHd), or delay time between the moment the input signal crosses the
switching level H to L and the zero crossing of the falling edge of the differential
output signal (tPDLd).
tOD-disp Input Overdrive Dispersion Change in tPD for different overdrive voltages at the input pins.
tSR-disp Input Slew Rate Dispersion Change in tPD for different slew rates at the input pins.
tCM-disp Input Common Mode Dispersion Change in tPD for different common mode voltages at the input pins.
ΔtPDLH resp
ΔtPDHL
Q to Q Time Skew Time skew between 50% levels of the rising edge of Q output and the falling
edge of output (ΔtPDLH), or time skew between 50% levels of falling edge of
Q output and rising edge of Q output (ΔtPDHL).
ΔtPD Average Q to Q Time Skew Average of tPDLH and tPDHL for L to H and H to L transients.
ΔtPDd Average Diff. Time Skew Average of tPDHd and tPDLd for L to H and H to L transients.
tr / trd Output Rise Time (20% - 80%) Time needed for the (single ended or differential) output voltage to change
from 20% of its nominal value to 80%.
tf / tfd Output Fall Time (20% - 80%) Time needed for the (single ended or differential) output voltage to change
from 80% of its nominal value to 20%.
tsLE Latch Setup Time Time the input signal has to be stable before enabling the latch functionality.
thLE Latch Hold Time Time the input signal has to remain stable after enabling the latch functionality.
tPD-LE Latch to Output Delay Time Delay time between the moment the latch input crosses the switching level H
to L and the moment the differential output signal crosses the 50% level.
Note: input signal is opposite to output signal when latch becomes enabled.
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LMH7322
20183204
FIGURE 3. Timing Definitions
20183203
FIGURE 4. LE Timing
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LMH7322
Pin Descriptions
Pin Name Description Comment
1. VCCOA Positive Supply Output Stage part A The supply pin for the output stage is independent of the supply
pin for the input pin. This allows output levels of different logic
families.
2. LEA Latch Enable Input part A Logic ‘1’ sets the part on hold. Logic levels are RSPECL (Reduced
Swing PECL) compatible.
3. LEA Latch Enable Input Not part A Logic ‘0’ sets the part on hold. Logic levels are RSPECL
compatible.
4. VEEA Negative Supply part A The supply pin for the negative supply is connected to the VEEB
via a string of two anti-parallel diodes (see Figure 1)
5. VCCIA Positive Supply for Input
Stage
part A The supply pin for the input stage is independent of the supply for
the output stage.
6. RHYSA Hysteresis Resistor part A The hysteresis voltage is determined by connecting a resistor from
this pin to RHREFA.
7. INA- Negative Input part A Input for analog voltages between 200 mV below VEEA and 2V
below VCCIA.
8. INA+ Positive Input part A Input for analog voltages between 200 mV below VEEA and 2V
below VCCIA.
9. RHREFA Reference Voltage Hysteresis
Resistor
part A The hysteresis voltage is determined by connecting a resistor from
this pin to RHYSA.
10. RHREFB Reference Voltage Hysteresis
Resistor
part B The hysteresis voltage is determined by connecting a resistor from
this pin to RHYSB.
11. INB+ Positive Input part B Input for analog voltages between 200 mV below VEEB and 2V
below VCCIB.
12. INB− Negative Input part B Input for analog voltages between 200 mV below VEEB and 2V
below VCCIB.
13. RHYSB Hysteresis Resistor part B The hysteresis voltage is determined by connecting a resistor from
this pin to RHREFB.
14. VCCIB Positive Supply for Input
Stage
part B The supply pin for the input stage is independent of the supply for
the output stage.
15. VEEB Negative Supply part B The supply pin for the negative supply is connected to the VEEA
via a string of two anti-parallel diodes (see Figure 1).
16. LEB Latch Enable Input Not part B Logic ‘0’ sets the part on hold. Logic levels are RSPECL
compatible.
17. LEB Latch Enable Input Logic part B 1’ sets the part on hold. Logic levels are RSPECL compatible.
18. VCCOB Positive Supply for Output
Stage
part B The supply pin for the output stage is independent of the supply
pin for the input pin. This allows output levels of different logic
families.
19. QB Inverted Output part B Output levels are determined by the choice of VCCOB.
20. QB Output part B Output levels are determined by the choice of VCCOB.
21. VCCOB Positive Supply for Output
Stage
part B See other VCCOB
22. VCCOA Positive Supply for Output
Stage
part A See other VCCOA.
23. QA Output part A Output levels are determined by the choice of VCCOA.
24. QA Inverted Output part A Output levels are determined by the choice of VCCOA.
25. DAP Central pad at the bottom of
the package
A & B This pad is connected to the VEE pins and its purpose is to transfer
heat outside the part.
www.national.com 16
LMH7322
TIPS & TRICKS USING THE LMH7322
In this section several aspects are discussed concerning spe-
cial applications using the LMH7322.
This concerns the LE function, the connection of the DAP in
conjunction to the VEE pins and the use of this part as an in-
terface between several logic families.
THE LATCH ENABLE PINS
The latch function is intended to stop the device from com-
paring the signals on both input pins. If the latch function is
enabled, the output is frozen and the logic information on the
output pins, present at that moment, is held until the latch
function is disabled. The timing of this process can be seen
in Figure 4. The input levels for the latch pins should comply
with RSPECL, but can also be driven with PECL type of sig-
nals if the minimum supply (VCCO –VEE) is larger or equal to
3.3V. The minimum differential latch input voltage should be
100 mV. Another possibility to set the LE function in a steady
state is to connect the pins via a resistor to the power supply.
If the LE pin is connected to VEE via a resistor of 10 k and
the LE-not pin is connected via 10 k to the VCCO pin the part
is continuously on. Since the latch input stage is referenced
to VCCO, the resistors to set the LE function should be con-
nected to this voltage. This is very important when working
with different voltages for VCCI and VCCO. If connected to the
wrong supply, the latch function will not work.
THE DAP AND THE VEE PINS
To ensure that both VEE pins are operating at the same volt-
age, both pins are connected to the DAP, and thus to each
other, through bond wires. As a consequence, the DAP is at
the same potential as the VEE pins and can be used to con-
nect the device to the minimum supply voltage. A more solid
VEE connection is obtained if the two VEE pins and the DAP
are all connected to the minimum supply on the PCB, rather
than an indirect connection through the internal bond wires.
To protect the device during handling and production two anti-
parallel connected diodes are connected between both VEE
pins. Under normal operating conditions these diodes are
shorted via the DAP.
The DAP (Die Attach Paddle) functions as a heat sink which
means that heat can be transferred using vias below this pad
to the copper plane VEE is connected to.
20183225
FIGURE 5. DAP Connection
INTERFACE BETWEEN LOGIC FAMILIES
As can be seen in the typical schematics (see the first part of
the datasheet) the LMH7322 can be used to interface be-
tween different logic families. The feature that facilitates this
property is the fact that the input stage and the output stage
use different positive power supply pins which can be used at
different supply voltages. The negative supply pins are con-
nected together for both parts. Using the power pins at differ-
ent supply voltages makes it possible to create several
translations for logic families. It is possible to translate from
logic at negative voltage levels such as ECL to logic at positive
levels such as RSPECL and LVDS and vice versa. The draw-
ings in the next paragraphs do not show the output resistors
except the first one. This is intentionally done for simplicity.
All outputs need an output resistor to a termination voltage or
to the negative rail as can be seen on the front page in the
typical application of an ECL to RSPECL converter.
Interface from ECL to RSPECL
The supply pin VCCI can be connected to ground because the
input levels are negative and the VCCO pin must operate at 5V
to create the RSPECL levels (see Figure 6). When working
with ECL, the negative supply pin (VEE) can be connected to
the −5.2V ECL supply voltage.
20183205
FIGURE 6. ECL TO RSPECL
17 www.national.com
LMH7322
Interface from PECL to (RS)ECL
The conversion from PECL to RS-ECL is possible when con-
necting the VCCI pin to +5V, which allows the input stage to
handle these positive levels. The VCCO pin must be connected
to the ground level in order to create the RSECL levels. The
high level of the output of the LMH7322 is normally 1.1V below
the VCCO supply voltage, and the low level is 1.5V below this
supply. The output levels are now −1100 mV for the logic ‘1’
and −1500 mV for the logic ‘0’ (see Figure 7). In the same way
the VEE can be connected to the ECL supply voltage of −5.2V.
20183206
FIGURE 7. PECL TO RSECL
Interface from Analog to LVDS
As seen in Figure 8, the LMH7322 can be configured to create
LVDS levels. This is done by connecting the VCCO to 2.5V. As
discussed before the output levels are now at VCCO –1.1V for
the logic ‘1’ and at VCCO −1.5V for the logic ‘0’. These levels
of 1000 mV and 1400 mV comply with the LVDS levels. As
can be seen in this setup, an AC coupled signal via a trans-
mission line is used. This signal is terminated with 50Ω.
20183207
FIGURE 8. ANALOG TO LVDS
Figure 9 shows a standard comparator setup which creates
RSPECL levels because the VCCO supply voltage is +5V. In
this case the VEE pin is connected to the ground level. The
VCCI pin is connected to the VCCO pin because there is no
need to use different positive supply voltages. The input sig-
nal is AC coupled to the positive input. To maintain reliable
results the input pins IN+ and IN− are biased at 1.4V through
a resistive divider using a resistor of 1 k to ground and a
resistor of 2.5 k to the VCC and by adding two decoupling
capacitors. Both inputs are connected to the bias level by the
www.national.com 18
LMH7322
use of a 10 k resistor. With this input configuration the input
stage can work in a linear area with signals of approximately
3 VPP (see input level restrictions in the data tables.)
20183208
FIGURE 9. Standard Setup
DELAY AND DISPERSION
Comparators are widely used to connect the analog world to
the digital one. The accuracy of a comparator is dictated by
its DC properties, such as offset voltage and hysteresis, and
by its timing aspects, such as rise and fall times and delay.
For low frequency applications most comparators are much
faster than the analog input signals they handle. The timing
aspects are less important here than the accuracy of the input
switching levels. The higher the frequencies, the more impor-
tant the timing properties of the comparator become, because
the response of the comparator can make a noticeable
change in critical parameters such as time frame or duty cy-
cle. A designer has to know these effects and has to deal with
them. In order to predict what the output signal will do, several
parameters are defined which describe the behavior of the
comparator. For a good understanding of the timing parame-
ters discussed in the following section, a brief explanation is
given and several timing diagrams are shown for clarification.
PROPAGATION DELAY
The propagation delay parameter is described in the definition
section. Due to this definition there are two parameters, tPDH
and tPDL (Figure 10). Both parameters do not necessarily have
the same value. It is possible that differences will occur due
to a different response of the internal circuitry. As a derivative
of this effect another parameter is defined: ΔtPD. This param-
eter is defined as the absolute value of the difference between
tPDH and tPDL.
20183211
FIGURE 10. Propagation Delay
If ΔtPD is not zero, duty cycle distortion will occur. For example
when applying a symmetrical waveform (e.g. a sinewave) at
the input, it is expected that the comparator will produce a
symmetrical square wave at the output with a duty cycle of
50%. When tPDH and tPDL are different, the duty cycle of the
output signal will not remain at 50%, but will be increased or
decreased. In addition to the propagation delay parameters
for single ended outputs discussed before, there are other
parameters in the case of complementary outputs. These pa-
rameters describe the delay from input to each of the outputs
and the difference between both delay times (See Figure
11.) When the differential input signal crosses the reference
level from L to H, both outputs will switch to their new state
with some delay. This is defined as tPDH for the Q output and
tPDL for the Q output, while the difference between both sig-
nals is defined as ΔtPDLH. Similar definitions for the falling
slope of the input signal can be seen in Figure 3.
19 www.national.com
LMH7322
20183212
FIGURE 11. tPD with Complementary Outputs
Both output circuits should be symmetrical. At the moment
one output is switching ‘on’ the other is switching ‘off’ with
ideally no skew between both outputs. The design of the
LMH7322 is optimized so that this timing difference is mini-
mized. The propagation delay, tPD, is defined as the average
delay of both outputs at both slopes: (tPDLH + tPDHL)/2.
Both overdrive and starting point should be equally divided
around the VREF (absolute values).
DISPERSION
There are several circumstances that will produce a variation
of the propagation delay time. This effect is called dispersion.
Amplitude Overdrive Dispersion
One of the parameters that causes dispersion is the amplitude
variation of the input signal. Figure 12 shows the dispersion
due to a variation of the input overdrive voltage. The overdrive
is defined as the ‘go to’ differential voltage applied to the in-
puts. Figure 12 shows the impact it has on the propagation
delay time if the overdrive is varied from 10 mV to 100 mV.
This parameter is measured with a constant slew rate of the
input signal.
20183213
FIGURE 12. Overdrive Dispersion
The overdrive dispersion is caused by the switching currents
in the input stage which is dependent on the level of the dif-
ferential input signal.
Slew Rate Dispersion
The slew rate is another parameter that affects propagation
delay. The higher the input slew rate, the faster the input stage
switches (See Figure 13).
20183214
FIGURE 13. Slew Rate Dispersion
A combination of overdrive and slew rate dispersion occurs
when applying signals with different amplitudes at constant
frequency. A small amplitude will produce a small voltage
change per time unit (dV/dt) but also a small maximum switch-
ing current (overdrive) in the input transistors. High ampli-
tudes produce a high dV/dt and a larger overdrive.
www.national.com 20
LMH7322
Common Mode Dispersion
Dispersion will also occur when changing the common mode
level of the input signal (Figure 14). When VREF is swept
through the CMVR (Common Mode Voltage Range), It results
in a variation of the propagation delay time. This variation is
called Common Mode Dispersion.
20183215
FIGURE 14. Common Mode Dispersion
All of the dispersion effects described previously influence the
propagation delay. In practice the dispersion is often caused
by a combination of more than one varied parameter.
HYSTERESIS & OSCILLATIONS
In contrast to an op amp, the output of a comparator has only
two defined states ‘0’ or ‘1.’ Due to finite comparator gain
however, there will be a small band of input differential voltage
where the output is in an undefined state. An input signal with
fast slopes will pass this band very quickly without problems.
During slow slopes however, passing the band of uncertainty
can take a relatively long time. This enables the comparators
output to switch back and forth several times between ‘0’ and
‘1’ on a single slope. The comparator will switch on its input
noise, ground bounce (possible oscillations), ringing etc.
Noise in the input signal will also contribute to these undesired
switching actions. The next sections explain these phenom-
ena in situations where no hysteresis is applied, and discuss
the possible improvement hysteresis can give.
Using No Hysteresis
Figure 15 shows what happens when the input signal rises
from just under the threshold VREF to a level just above it.
From the moment the input reaches the lowest dotted line
around VREF at t=0, the output toggles on noise etc. Toggling
ends when the input signal leaves the undefined area at t=1.
In this example the output was fast enough to toggle three
times. Due to this behavior digital circuitry connected to the
output will count a wrong number of pulses. One way to pre-
vent this is to choose a very slow comparator with an output
that is not able to switch more than once between ‘0’ and ‘1’
during the time the input state is undefined.
20183216
FIGURE 15. Oscillations on Output Signal
In most circumstances this is not an option because the slew
rate of the input signal will vary.
Using Hysteresis
Hysteresis can be introduced to avoid oscillations, e.g. due to
noise on the input signal, especially for slow edges. For this
purpose the switching level without hysteresis (VREF) is forced
to a new level (A or B) at the moment the input signal crosses
one of these levels. This can be seen in Figure 16.
20183218
FIGURE 16. Hysteresis
In this picture the two dotted lines A and B, represent the re-
sulting reference level at which the comparator will compare
the input level against. Assume that for this situation the input
signal is connected to the negative input and the switching
level (VREF) to the positive input. The input level drawn in
Figure 16 starts much lower as the reference level and this
means that the input stage is well defined with the inverting
input much lower than the non-inverting input. As a result the
output will be in the high state. Internally the switching level
is at level A, with the input signal sloping up, this situation
remains until VIN crosses level A at t=1. Now the output tog-
gles, and the internal switching level is lowered to level B. So
before the output has the possibility to toggle again, the volt-
age difference between the inputs is sufficient to have a stable
situation again. When the input signal comes down from high
21 www.national.com
LMH7322
to low, the situation is stable until level B is reached at t=0. At
this moment the output will toggle back, and the circuit returns
to the starting situation with the inverting input at a much lower
level than the non inverting input. Varying the levels A and B
due to the change of the hysteresis resistor will also vary the
timing of t=0 and t=1. When designing a circuit be aware of
this effect. Introducing hysteresis will cause some time shift
between output and input (e.g. duty cycle variations), but will
eliminate undesired switching of the output.
Configuring Hysteresis for the LMH7322
The LMH7322 offers the possibility to introduce hysteresis by
connecting a resistor between the RHYS pin and the RHREF
pin. This hysteresis setting resistor may vary between zero
ohm and infinite. The current drawn from the RHYS pin de-
termines the setting of the internal reference voltage. When
no resistor is present the internal used reference voltage is
set to zero (the difference between A and B level is zero, see
explanation Using Hysteresis) and no hysteresis is config-
ured. This means the output will change state when the
difference between the positive en negative input signals
crosses zero level. Connecting a resistor between the RHYS
pin and the RHREF pin produces a difference for the A and
B levels which means hysteresis is introduced and the output
will change state at different levels for an up or down transition
of the input signal. Due to the internal structure a current must
be drawn from the RHYS pin. This can be done by connecting
a resistor to the lowest supply voltage. In order to assure the
RHYS pin is connected to the correct voltage level, and un-
wanted current variations in the hysteresis level are avoided,
the RHREF and VEE are connected internally within the
LMH7322. Therefore, the hysteresis resistor should only be
connected between RHYS and RHREF or left open if no hys-
teresis is required. To select the correct resistor for the de-
sired hysteresis voltage see Figure 17.
20183239
FIGURE 17. Hysteresis Voltage vs. Hysteresis Resistor
With the use of a resistor to set the hysteresis voltage no ex-
ternal conditions will effect these setting as long as they stay
within the normal operating ranges. Temperature changes
may cause a variation of the hysteresis resistor dictated by
the temperature coefficient of the used type. Connecting the
RHYS pin to another voltage as provided by the RHREF pin
is not covered in the resistor selection plot and the designer
of such a circuit must be aware of abnormal behavior.
The Output
OUTPUT SWING PROPERTIES
The LMH7322 has differential outputs which means that both
outputs have the same swing but in opposite directions (See
Figure 18). Both outputs swing around the common mode
output voltage (VO). This voltage can be measured at the
midpoint between two equal resistors connected to each out-
put. The absolute value of the difference between both volt-
ages is called VOD. The outputs cannot be held at the VO level
because of their digital nature. They only cross this level dur-
ing a transition. Due to the symmetrical structure of the circuit,
both output voltages cross at VO regardless of whether the
output changes from ‘0’ to ‘1’ or vise versa.
20183219
FIGURE 18. Output Swing
LOADING THE OUTPUT
Both outputs are activated when current is flowing through a
resistor that is externally connected to VT. The termination
voltage should be set 2V below the VCCO. This makes it pos-
sible to terminate each of the outputs directly with 50, and
if needed to connect through a transmission line with the
same impedance (see Figure 19). Due to the low ohmic na-
ture of the output emitter followers and the 50 load resistor,
a capacitive load of several pF does not dramatically affect
the speed and shape of the signal. When transmitting the sig-
nal from one output to any input the termination resistor
should match the transmission line. The capacitive load (CP)
will distort the received signal. When measuring this input with
a probe, a certain amount of capacitance from the probe is
parallel to the termination resistor. The total capacitance can
be as large as 10 pF. In this case there is a pole at:
f = 1/(2*π*C*R)
f = 1e9/ π
f = 318 MHz
In this case the current IP has the same value as the current
through the termination resistor. This means that the voltage
drops at the input and the rise and fall times are dramatically
different from the specified numbers for this part.
Another parasitic capacitance that can affect the output signal
is the capacitance directly between both outputs, called
CPAR (see Figure 19). The LMH7322 has two complementary
outputs so there is the possibility to transport the output signal
by a symmetrical transmission line. In this case both output
tracks form a coupled line with their own parasitics and both
receiver inputs connected to the transmission line. Actually
the line termination looks like 100 and the input capaci-
tances, which are in series, are parallel to the 100 termina-
tion. The best way to measure the input signal is to use a
differential probe directly across both inputs. Such a probe is
very suitable for measuring these fast signals because it has
good high frequency characteristics and low parasitic capac-
itance.
www.national.com 22
LMH7322
20183221
FIGURE 19. Parasitic Capacitance
TRANSMISSION LINES & TERMINATION
TECHNOLOGIES
The LMH7322 uses complementary RSPECL outputs and
emitter followers, which means high output current capability
and low sensitivity to parasitic capacitance. The use of Re-
duced Swing Positive Emitter Coupled Logic reduces the
supply voltage to 2.7V, being the lowest possible value, and
raises the maximum frequency response. Data rates are
growing, which requires increasing speed. Data is not only
connected to other IC’s on a single PCB board but, in many
cases, there are interconnections from board to board or from
equipment to equipment. Distances can be short or long but
it is always necessary to have a reliable connection, which
consumes low power and is able to handle high data rates.
The complementary outputs of the LMH7322 make it possible
to use symmetrical transmission lines The advantage over
single ended signal transmission is that the LMH7322 has
higher immunity to common mode noise. Common mode sig-
nals are signals that are equally apparent on both lines and
because the receiver only looks at the difference between
both lines, this noise is canceled.
Maximum Bit Rates
The maximum toggle rate is defined at an amplitude of 50%
of the nominal output signal. This toggle rate is a number for
the maximum transfer rate of the part and can be given in Hz
or in Bps. When transmitting signals in a NRZ (Non Return to
Zero) format the bitrate is double this frequency number, be-
cause during one period two bits can be transmitted. (See
Figure 20.) The rise and fall times are very important specifi-
cations in high speed circuits. In fact these times determine
the maximum toggle rate of the part. Rise and fall times are
normally specified at 20% and 80% of the signal amplitude
(60% difference). Assuming that the edges at 50% amplitude
are coming up and down like a sawtooth it is possible to cal-
culate the maximum toggle rate but this number is too opti-
mistic. In practice the edges are not linear while the pulse
shape is more or less a sinewave.
20183222
FIGURE 20. Bit Rates
Need for Terminated Transmission Lines
During the 1980’s and 90’s, National fabricated the 100K ECL
logic family. The rise and fall time specifications were 0.75 ns,
which are considered very fast. If sufficient care has not been
given in designing the transmission lines and choosing the
correct terminations, then errors in digital circuits are intro-
duced. To be helpful to designers that use ECL with “old”
PCB-techniques, the 10K ECL family was introduced with a
rise and fall time specification of 2 ns. This was much slower
and easier to use. The RSPECL output signals of the
LMH7322 have transition times that extend the fastest ECL
family. A careful PCB design is needed using RF techniques
for transmission and termination. Transmission lines can be
formed in several ways. The most commonly used types are
the coaxial cable and the twisted pair telephony cable (Figure
21).
20183223
FIGURE 21. Cable Types
23 www.national.com
LMH7322
These cables have a characteristic impedance determined by
their geometric parameters. Widely used impedances for the
coaxial cable are 50 and 75. Twisted pair cables have
impedances of about 120 to 150Ω.
Other types of transmission lines are the strip line and the
micro strip line. These last types are used on PCB boards.
They have the characteristic impedance dictated by the phys-
ical dimensions of a track placed over a metal ground plane
(see Figure 22).
20183224
FIGURE 22. PBC Lines
Differential Microstrip
Line The transmission line which is ideally suited for comple-
mentary signals is the differential microstrip line. This is a
double microstrip line with a narrow space in between. This
means both lines have strong coupling and this determines
the characteristic impedance. The fact that they are routed
above a copper plane does not affect differential impedance,
only CM-capacitance is added. Each of the structures above
has its own geometric parameters, so for each structure there
is different formula to calculate the right impedance. For cal-
culations on these transmission lines visit the National web-
site or order RAPIDESIGNER. At the end of the transmission
line there must be a termination having the same impedance
as that of the transmission line itself. It does not matter what
impedance the line has, if the load has the same value no
reflections will occur. When designing a PCB board with
transmission lines on it, space becomes an important item
especially on high density boards. With a single microstrip
line, line width is fixed for given impedance and a board ma-
terial. Other line widths will result in different impedances.
Advantages of Differential MicrostripLines
Impedances of transmission lines are always dictated by their
geometric parameters. This is also true for differential mi-
crostrip lines. Using this type of transmission line, the distance
of the track determines the resulting impedance. So, if the
PCB manufacturer can produce reliable boards with low track
spacing the track width for a given impedance is also small.
The wider the spacing, the wider tracks are needed for a spe-
cific impedance. For example two tracks of 0.2 mm width and
0.1 mm spacing have the same impedance as two tracks of
0.8 mm width and 0.4 mm spacing. With high-end PCB pro-
cesses, it is possible to design very narrow differential mi-
crostrip transmission lines. It is desirable to use these to
create optimal connections to the receiving part or the termi-
nating resistor, in accordance to their physical dimensions.
Seen from the comparator, the termination resistor must be
connected at the far end of the line. Open connections after
the termination resistor (e.g. to an input of a receiver) must
be as short as possible. The allowed length of such connec-
tions varies with the received transients. The faster the tran-
sients, the shorter the open lines must be to prevent signal
degradation.
PCB LAYOUT CONSIDERATIONS AND COMPONENT
VALUE SELECTION
High frequency designs require that both active and passive
components be selected from those that are specially de-
signed for this purpose. The LMH7322 is fabricated in a 24-
pin LLP package intended for surface mount design. For
reliable high speed design it is highly recommended to use
small surface mount passive components because these
packages have low parasitic capacitance and low inductance
simply because they have no leads to connect them to the
PCB. It is possible to amplify signals at frequencies of several
hundreds of MHz using standard through-hole resistors. Sur-
face mount devices however, are better suited for this pur-
pose. Another important issue is the PCB itself, which is no
longer a simple carrier for all the parts and a medium to in-
terconnect them. The PCB becomes a real component itself
and consequently contributes its own high frequency proper-
ties to the overall performance of the circuit. Good practice
dictates that a high frequency design have at least one ground
plane, providing a low impedance path for all decoupling ca-
pacitors and other ground connections. Care should be given
especially that on-board transmission lines have the same
impedance as the cables to which they are connected. Most
single ended applications have 50 impedance (75 for
video and cable TV applications). Such low impedance, single
ended microstrip transmission lines usually require much
wider traces (2 to 3 mm) on a standard double sided PCB
board than needed for a ‘normal’ trace. Another important is-
sue is that inputs and outputs should not ‘see’ each other. This
occurs if input and output tracks are routed in parallel over the
PCB with only a small amount of physical separation, partic-
ularly when the difference in signal level is high. Furthermore,
components should be placed as flat and low as possible on
the surface of the PCB. For higher frequencies a long lead
can act as a coil, a capacitor or an antenna. A pair of leads
can even form a transformer. Careful design of the PCB min-
imizes oscillations, ringing and other unwanted behavior. For
ultra high frequency designs only surface mount components
will give acceptable results. (For more information see
OA-15).
NSC suggests the following evaluation board as a guide for
high frequency layout and as an aid in device testing:
LMH7322EVAL
www.national.com 24
LMH7322
Physical Dimensions inches (millimeters) unless otherwise noted
24-Pin LLP Package
NS Package Number SQA24A
25 www.national.com
LMH7322
Notes
LMH7322 Dual 700 ps High Speed Comparator with RSPECL Outputs
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